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HTPD Monterey, CA 7-11 May 2012 F.Volpe 1
F. Volpe1, M.E. Austin2, G. Campbell3, T. Deterly3
1 Columbia University, New York2 University of Texas, Austin3 General Atomics, San Diego
Oblique-ECE Radial and Phase Detector of Rotating Magnetic Islands applied
to Alignment and Phase-locked Modulation of ECCD for NTM Stabilization
19th Topical Conference
High-Temperature Plasma Diagnostics
Monterey, CA, May 6-10, 2012
Yosemite, Sept.2006
HTPD Monterey, CA 7-11 May 2012 F.Volpe 2
Abstract
A 2 channel oblique Electron Cyclotron Emission (ECE) radiometerinterfaced to 4 gyrotrons was used at DIII-D to toroidally and radiallylocalize rotating magnetic islands and so assist their Electron CyclotronCurrent Drive (ECCD) stabilization. In particular, after manipulationsoperated by the interfacing analogue circuit, the oblique ECE signalsdirectly modulated the current drive in synch with the island rotation and inphase with the island O-point, for a more efficient stabilization. Apart fromthe different toroidal location, the diagnostic view was identical to theECCD launch direction, which greatly simplified the use in real time of thesignals. In fact, a simple toroidal extrapolation was sufficient to lock theECCD modulation to the O-point phase. This was accomplished by aspecially designed phase-shifter of flat response over the 1-7kHz range.Moreover, correlation analysis of two oblique ECE channels slightly aboveand below the ECCD frequency permitted to check the radial alignment ofECCD to the island, based on the fact that for satisfactory alignment thetwo oblique ECE signals must be out of phase.
HTPD Monterey, CA 7-11 May 2012 F.Volpe 3
Why modulating ECCD?
To maximize CD in the island (stabilizing) vs. CD outside (destab.)
For fairly oblique (Doppler-broadened), staggered launch of gyrotron beams, AUG and DIII-D can reproduce ITER-like conditions: w< dECCD
(narrow CD)
(broad CD)
dECCD
HTPD Monterey, CA 7-11 May 2012 F.Volpe 4
Why ECE (and not magnetic probes)?Because it is local toroidal phase & radial localization
• Mirnov:
++ Frequency
• ECE:
+ Frequency
0.0 0.2 0.4 0.6 0.8 1.0time (ms) – 4550.
• Mirnov:++ Frequency
+ Phase (measurement not local,
requires helical extrapolation)
−− Radial alignment
• ECE:+ Frequency
++ Phase (local but, if not in situ,
requires helical extrapolation)
++ Radial alignmentT
e(k
eV
) B
p(a
.u.)
MIRNOV
ECE 86.5GHz
125658
M.Marascheck et al. PRL 2007
rotation
HTPD Monterey, CA 7-11 May 2012 F.Volpe 5
Oblique ECE, along same direction as ECCD no equilibrium or other analysis required
• Island transit measured ‘in situ’
– same R, z of CD
– from same R, z of ECRH launcher
– with same pol. & tor. view angles
• Hence
– same relativistic downshift
– same relativistic & Doppler broadening
– island centre emits at f=fgyr=110GHz
• No need for FFT
• No need for flux surface shape
or helical extrapolations in R,z,f.
Extrapolation only in f.
• Horizontal ECE at 110GHz suffers from 3rd harm.
problems for BT<1.65T, oblique ECE only BT<1.55T
#125476
t=3750ms
B= -1.7T
#122898
t=5000ms
B= -1.5T
HTPD Monterey, CA 7-11 May 2012 F.Volpe 6
Oblique ECE from rotating island collected by transmission line 5
Modulated ECCD injected from lines 2, 3, 4 & 6 to stabilize island
fECCD ≠ fgyr but Df =15, 30, 330, 345o anyway
HTPD Monterey, CA 7-11 May 2012 F.Volpe 7
Island separatrix is an isothermal.
Signals on island sides are out-of-phase.
dTe in counter-phase
Same Te
(changes with time)Loc
Max
Loc
min
r3/2
MSE
0 0.5 1.0 r
4
2
0
Te(keV)
HTPD Monterey, CA 7-11 May 2012 F.Volpe 8
Two ECE channels close to island are sufficient to
track its rotation and radially localize it w.r.t. ECCD
ECE @ outer edge of island
ECE @ inner edge of island
Diff. of two horiz. ECE channels
MECCD w/form (apart from phase)
r 86.5GHz
88.5GHz
Mirnov
MECCD w/form (apart from phase)
HTPD Monterey, CA 7-11 May 2012 F.Volpe 9
Channels on opposite sides of island (mid-frequency aligned) out-of-phase
Channels on same side (mid-frequency misaligned) in phase
r 88.5GHz
90.5GHz
85.5GHz
87.5GHz
HTPD Monterey, CA 7-11 May 2012 F.Volpe 10
Oblique ECE as a waveform generator for modulated ECCD,
radially aligned, in synch and in phase with island O-point
Doppler-broadened,
relativistically shifted
111.5 108.5GHz ECRs
RM FiltersSubtractor/
Comparator
V1
V2
Analog Processing Freq & Phase of Modulation
Optical
Isolator
fibrePS Gyrotron
Optical
Isolator
fibrePS Gyrotron
Optical
Isolator
fibrePS Gyrotron
+Df
+Df
PCS
Digital Processing Radius of CD
(if wrong, move plasma or ECR)
HTPD Monterey, CA 7-11 May 2012 F.Volpe 11
Dichroic plate and plate array
Frequency selectivity
(no mix-up with LFS)
Modal Purity
(no mix-up with O-mode)
HTPD Monterey, CA 7-11 May 2012 F.Volpe 12
Analogue circuit modulates ECCD based on oblique ECE
and corrects phase for different toroidal location
Subtractor ComparatorPhase
ShifterV1-V2
V1
V2
300Hz < f < 20kHz
FilterV1-V2
• Phase shifters usually provide fixed time delay
• Special design: flat frequency response in phase
Frequency
to Voltage
Converter
Programmable
Voltage Controlled
Resistor
V
f
R 1/V 1/f
Dt=RC 1/f
but Df=const.
200
400
600
800
1000
0 2 4 6 8
f (kHz)
D
Df d
Dt (s)
Df (deg)
HTPD Monterey, CA 7-11 May 2012 F.Volpe 13
Gyrotrons are modulated at up to 10kHz
Balanced NBI slows down rotation to ITER-like valuesP
EC
RH(M
W)
f=10kHz
f=2kHz
time (s)
25
20
15
10
5
01.8 2.62.2 3.0 3.4 3.8
3/2, 4kHz
f (k
Hz)
HTPD Monterey, CA 7-11 May 2012 F.Volpe 14
Observed Phase Reversal, indication of good alignment !
HTPD Monterey, CA 7-11 May 2012 F.Volpe 15
Complete suppression of 3/2 by ECCD modulated
in phase with O-point !
HTPD Monterey, CA 7-11 May 2012 F.Volpe 16
Complete suppression of 3/2
is well separated from appearance of 2/1
HTPD Monterey, CA 7-11 May 2012 F.Volpe 17
Summary and Conclusions
• Physical principle
– Oblique ECE tracks island along ECCD line of sight, toroidally shifted
– Signals directly modulate ECCD
– Radial alignment in real-time, from 2 channel anti-correlation
• Demonstrated both techniques!
1. Observed “Phase-reversal”, indication of good alignment
• confirmed by 3/2 stabilization and by equilibrium and ray tracing
analysis
2. 3/2 NTM completely suppressed by ECCD modulated in phase
with O-point on the basis of oblique ECE signals
HTPD Monterey, CA 7-11 May 2012 F.Volpe 18
Future Works
• Stabilize 2/1
• Align in real-time
• Compare with Mirnov
• Oblique radiometer might also serve to:
– EBW emission
– Collective Thomson Scattering
– Correlation with horizontal ECE ( toroidal mode number)
– Positron Cyclotron Emission
• Electronics can be used with any NTM diagnostic